Search results for "Collision"

showing 10 items of 908 documents

Measurement of upsilon production in 7 TeV pp collisions at ATLAS

2013

Artículo escrito por un elevado número de autores, solo se referencian el que aparece en primer lugar, el nombre del grupo de colaboración, si le hubiere, y los autores pertenecientes a la UAM

Prompt J/Psi ProductionUpsilon meson01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Polarization[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentQCQuantum chromodynamicsPhysicsLarge Hadron ColliderHeavy QuarkoniumSettore FIS/01 - Fisica SperimentaleCharmonium ProductionATLASJ-PsiHelicityLarge Hadron ColliderHadronic CollisionsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGLHCpp collisionsParticle Physics - ExperimentNuclear and High Energy PhysicsParticle physicsMesonCiências Naturais::Ciências Físicas530 PhysicsGluons:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2upsilon production; pp collisions ; ATLAS; detector530Nuclear physics0103 physical sciencesddc:530RapidityHigh Energy Physics010306 general physicsScience & TechnologyATLAS detector010308 nuclear & particles physicsBranching fractionFísicaQCDGluonOctet Quarkonia ProductionHADRON-HADRON COLLISIONSRoot-S=7 TevExperimental High Energy PhysicsHigh Energy Physics::ExperimentHeavy quarkonia
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Search for new particles in two-jet final states in 7 TeV proton-proton collisions with the ATLAS detector at the LHC

2010

19 páginas, 2 figuras, 1 tabla.-- et al.(ATLAS Collaboration).

ProtonAtlas detectorPhysics::Instrumentation and DetectorsPhysics beyond the Standard ModelGeneral Physics and AstronomyJet (particle physics)particle physic01 natural sciencesSettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)12.60.Rcddc:550[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]13.87.CeQCPhysicsPACS numbers: 13.85.Rm 12.60.Rc 13.87.Ce 14.80.-jLarge Hadron ColliderLuminosity (scattering theory)Cross sectionAcceleradors de partículesSettore FIS/01 - Fisica Sperimentale14.80.-jATLASnumbers: 13.85.Rm3. Good healthDijetsmedicine.anatomical_structureComputingMethodologies_DOCUMENTANDTEXTPROCESSINGTWO-JETSLHCParticle Physics - ExperimentjetsFinal stateParticle physicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Partícules (Física nuclear)Nuclear physicsCross section (physics)Excited QuarksAtlas (anatomy)0103 physical sciencesmedicine010306 general physicsIntegrated luminosityProton proton collisionsParton Distributions010308 nuclear & particles physicsATLAS detectorsHigh Energy Physics::PhenomenologyFísicaPARTON DISTRIBUTIONS HADRON COLLIDERS EXCITED QUARKS DIJETSHadron CollidersHeavy particlesLHC ; ATLAS ; Collisions ; 7 TeV ; Two jets ; ResonancesExperimental High Energy PhysicsNEW PARTICLESproton-proton collisionsHigh Energy Physics::Experimentcollider
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Measurement of visible cross sections in proton-lead collisions at √sNN= 5.02 TeV in van der Meer scans with the ALICE detector

2014

In 2013, the Large Hadron Collider provided proton-lead and lead-proton collisions at the center-of-mass energy per nucleon pair $\sqrt{s_{\rm{NN}}}=5.02$ TeV. Van der Meer scans were performed for both configurations of colliding beams, and the cross section was measured for two reference processes, based on particle detection by the T0 and V0 detectors, with pseudo-rapidity coverage $4.6<\eta< 4.9$, $-3.3<\eta<-3.0$ and $2.8<\eta< 5.1$, $-3.7<\eta<-1.7$, respectively. Given the asymmetric detector acceptance, the cross section was measured separately for the two configurations. The measured visible cross sections are used to calculate the integrated luminosity of the proton-lead and lead-…

ProtonNuclear Theorylarge detector systems for particle and astroparticle physicsLarge detector systems for particle and astroparticle physics; Particle tracking detec- tors; Heavy-ion detectors01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Particle tracking detectorsparticle tracking detectors[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Neutron detectionNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentInstrumentationMathematical PhysicsPhysicsLarge Hadron ColliderLuminosity (scattering theory)PhysicsDetectorLuminosity measurement3. Good healthPRIRODNE ZNANOSTI. Fizika.Large detector systems for particle and astroparticle physics Particle tracking detec- torNucleonParticle Physics - ExperimentLarge detector systems for particle and astroparticle physics ; Particle tracking detectors ; Heavy-ion detectorsParticle physicsParticle tracking detec- torsInstrumentationHeavy-ion detectorsFOS: Physical sciencesLarge detector systems for particle and astroparticle physics; Particle tracking detectors; Heavy-ion detectors[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear physicsCross section (physics)p-Pb collisions at the LHC0103 physical sciencesNuclear Physics - Experiment010306 general physics010308 nuclear & particles physicsLarge detector systems for particle and astroparticle physicsALICE experimentLarge detector systems for particle and astroparticle physics Particle tracking detec- tors; Heavy-ion detectorsNATURAL SCIENCES. Physics.heavy-ion detectorsInstrumentation; Mathematical PhysicsPhysics::Accelerator PhysicsHigh Energy Physics::Experiment
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Measurement of multi-jet cross sections in proton-proton collisions at a 7 TeV center-of-mass energy

2011

Inclusive multi-jet production is studied in proton–proton collisions at a center-of-mass energy of 7 TeV, using the ATLAS detector. The data sample corresponds to an integrated luminosity of 2.4 pb−1. Results on multi-jet cross sections are presented and compared to both leading-order plus parton-shower Monte Carlo predictions and to next-to-leading-order QCD calculations.

ProtonPhysics and Astronomy (miscellaneous)EventsMonte Carlo methodJet (particle physics)01 natural sciences7. Clean energyHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentQuantum chromodynamicsPhysicsLuminosity (scattering theory)PhysicsSettore FIS/01 - Fisica SperimentaleHERAATLASINCLUSIVE JET CROSS SECTIONPhotoproductionmedicine.anatomical_structurePhysical SciencesFísica nuclearLHCParticle Physics - ExperimentSimulationParticle physicsCiências Naturais::Ciências FísicasAstrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Nuclear physicsAtlas (anatomy)0103 physical sciencesproton–proton collisions; center-of-mass energymedicineFysikddc:530High Energy Physics010306 general physicsEngineering (miscellaneous)HeraScience & Technology010308 nuclear & particles physicsAntiproton ColliderHADRON-HADRON COLLISIONSHigh Energy Physics::ExperimentCenter of mass
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Witnessing objectivity on a quantum computer

2021

Understanding the emergence of objectivity from the quantum realm has been a long standing issue strongly related to the quantum to classical crossover. Quantum Darwinism provides an answer, interpreting objectivity as consensus between independent observers. Quantum computers provide an interesting platform for such experimental investigation of quantum Darwinism, fulfilling their initial intended purpose as quantum simulators. Here we assess to what degree current NISQ devices can be used as experimental platforms in the field of quantum Darwinism. We do this by simulating an exactly solvable stochastic collision model, taking advantage of the analytical solution to benchmark the experime…

Quantum PhysicsPhysics and Astronomy (miscellaneous)Materials Science (miscellaneous)FOS: Physical sciences01 natural sciencesAtomic and Molecular Physics and OpticsSettore FIS/03 - Fisica Della Materia010305 fluids & plasmas0103 physical sciencesOpen quantum systems quantum darwinism quantum objectivityElectrical and Electronic Engineeringcollision models; objectivity; quantum computers; quantum Darwinism; quantum information010306 general physicsQuantum Physics (quant-ph)
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Extracting work from random collisions: A model of a quantum heat engine

2022

We study the statistical distribution of the ergotropy and of the efficiency of a single-qubit battery ad of a single-qubit Otto engine, respectively fuelled by random collisions. The single qubit, our working fluid, is assumed to exchange energy with two reservoirs, a non-equilibrium "hot" reservoir and a zero temperature cold reservoir. The interactions between the qubit and the reservoirs is described in terms of a collision model of open system dynamics. The qubit interacts with the non-equilibrium reservoir (a large ensemble of qudits all prepared in the same pure state) via random unitary collisions and with the cold reservoir (a large ensemble of qubits in their ground state) via a p…

Quantum PhysicsRandom collisionsCold working; Engines; Ground stateStatistical Mechanics (cond-mat.stat-mech)Quantum ThermodynamicsFOS: Physical sciencesQuantum PhysicsQuantum Physics (quant-ph)Settore FIS/03 - Fisica Della MateriaCondensed Matter - Statistical MechanicsPhysical Review E
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Influence of a temperature-dependent shear viscosity on the azimuthal asymmetries of transverse momentum spectra in ultrarelativistic heavy-ion colli…

2012

We study the influence of a temperature-dependent shear viscosity over entropy density ratio $\eta/s$, different shear relaxation times $\tau_\pi$, as well as different initial conditions on the transverse momentum spectra of charged hadrons and identified particles. We investigate the azimuthal flow asymmetries as a function of both collision energy and centrality. The elliptic flow coefficient turns out to be dominated by the hadronic viscosity at RHIC energies. Only at higher collision energies the impact of the viscosity in the QGP phase is visible in the flow asymmetries. Nevertheless, the shear viscosity near the QCD transition region has the largest impact on the collective flow of t…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsNuclear TheoryHadronElliptic flowFOS: Physical sciencesCollisionSpectral lineNuclear physicsPhysics::Fluid DynamicsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Shear (geology)Quark–gluon plasmaHigh Energy Physics::ExperimentCentralityNuclear Experiment
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Initial conditions of heavy ion collisions and small x

2009

The Color Glass Condensate (CGC), describing the physics of the nonlinear gluonic interactions of QCD at high energy, provides a consistent first-principles framework to understand the initial conditions of heavy ion collisions. This talk reviews some aspects of the initial conditions at RHIC and discusses implications for LHC heavy ion phenomenology. The CGC provides a way compute bulk particle production and understand recent experimental observations of long range rapidity correlations in terms of the classical glasma field in the early stages of the collision.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderHigh Energy Physics::PhenomenologyFOS: Physical sciencesCollisionColor-glass condensateNuclear physicsNonlinear systemHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quark–gluon plasmaRapidityNuclear ExperimentPhenomenology (particle physics)
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Measurement of the charged particle multiplicity distribution in hadronic Z decays

1991

The charged particle multiplicity distribution of hadronic Z decays was measured on the peak of the Z resonance using the ALEPH detector at LEP. Using a model independent unfolding procedure the distribution was found to have a mean = 20.85 +/- 0.24 and a dispersion D = 6.34 +/- 0.12. Comparison with lower energy data supports the KNO scaling hypothesis in the energy range square-root s = 29-91.25 GeV. At square-root s = 91.25 GeV the shape of the multiplicity distribution is well described by a log-normal distribution, as predicted from a cascading model for multi-particle production. The same model also successfully describes the energy dependence of the mean and width of the multiplicity…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsRange (particle radiation)Particle physicsE+E ANNIHILATIONPP COLLISIONSDistribution (number theory)Electron–positron annihilationQUARKHadronPETRA ENERGIESResonance (particle physics)Charged particleNuclear physicsMONTE-CARLOHigh Energy Physics::ExperimentFRAGMENTATIONScalingParticle Physics - Experiment
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Inclusive dijet photoproduction in ultraperipheral heavy ion collisions at the CERN Large Hadron Collider in next-to-leading order QCD

2019

We compute the cross section of inclusive dijet photoproduction in ultraperipheral Pb-Pb collisions at the CERN Large Hadron Collider using next-to-leading order perturbative QCD. We demonstrate that our theoretical calculations provide a good description of various kinematic distributions measured by the ATLAS Collaboration. We find that the calculated dijet photoproduction cross section is sensitive to nuclear modifications of parton distribution functions (PDFs) at the level of 10% to 20%. Hence, this process can be used to reduce uncertainties in the determination of these nuclear PDFs, whose current magnitude is comparable to the size of the calculated nuclear modifications of the dije…

Quantum chromodynamicsPhysicsPB-PB COLLISIONSParticle physicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyNuclear TheoryPerturbative QCDPartonhiukkasfysiikkaJ/PSI PHOTOPRODUCTION01 natural sciences114 Physical sciencesCROSS-SECTIONSPHYSICSDistribution functionHERA DIRECTRHO0103 physical sciencesHeavy ionHigh Energy Physics::Experiment010306 general physicsNuclear Experiment
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